Beam loss and radiation effects in the SSC lattice elements [electronic resource]
The Superconducting Super Collider (SSC) is designed to be an advanced machine with relatively low beam loss-induced radiation levels. However, a fraction of the beam lost in the lattice due to pp-collisions at the interaction points, beam-gas scattering, bearn-halo scraping, various instabilities a...
Saved in:
| Online Access: |
Online Access |
|---|---|
| Corporate Author: | |
| Format: | Government Document Electronic eBook |
| Language: | English |
| Published: |
Washington, D.C. : Oak Ridge, Tenn. :
United States. Dept. of Energy ; distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy,
1990.
|
| Subjects: |
| Summary: | The Superconducting Super Collider (SSC) is designed to be an advanced machine with relatively low beam loss-induced radiation levels. However, a fraction of the beam lost in the lattice due to pp-collisions at the interaction points, beam-gas scattering, bearn-halo scraping, various instabilities and errors will result in the irradiation of conventional and superconducting components of the accelerator and experimental apparatus. The level of the beam loss and its distribution along the machine structure has impact on all of the three crucial radiation effects at the SSC: quenching of the superconducting magnets, survivability of the accelerator and detectors components in the near-beam regions, and influence to the environment. This paper, based on the full-scale Monte Carlo simulation, will explore all major sources of beam loss in the Collider and measures to reduce the irradiation of the accelerator components. Basic parameters of the Super Collider accepted throughout this report are as follows: Proton energy E₀ = 20 TeV, injection energy is 2 TeV, number of protons circulating in each of the collider rings is N = 1.3 × 10¹⁴, circumference is 87.12 km, the transverse normalized emittance {var_epsilon}{sub N}(σ) = 1 π mm-mrad, for the regular lattice (β = 305 m) the beam R.M.S. sizes are σ = 0.12 mm at 20 TEV and σ = 0.38 mm at the injection energy. The dipole length is 15.815 m with the effective field length of 15.165 m. The magnetic field map for B₀ = 6.5999 T has been calculated with the POISSON program by Greg Snitchler. The turn angle of each dipole is α = 1.50027 mrad. The dipole aperture is 50 mm. The two beam pipe diameters are studied 33 and 40 mm. The operating temperature is T₀ = 4.35 K. |
|---|---|
| Item Description: | Published through the Information Bridge: DOE Scientific and Technical Information. 11/01/1990. "sscl--306" "DE95011790" Mokhov, N.V.; Drozhdin, A.I.; Baishev, I.S. |
| Physical Description: | 75 p. : digital, PDF file. |